In the absence of dissipative forces, the total mechanical energy of a simple harmonic oscillator is constant and proportional to the square of the amplitude:
"E = \\frac{1}{2}kA^2"
where the potential energy has been chosen to be zero at the equilibrium point. At any point, the sum of the kinetic and potential energies is constant:
"E = \\frac{1}{2}mv_x^2 + \\frac{1}{2}kx^2 = \\frac{1}{2}kA^2"
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